Let r be the radius of the capillary tube, h the rise of the liquid in the capillary, θ the angle of contact.
The liquid makes contact with the tube along a line of length 2πr . As the surface tension S acts tangentially to the liquid surface, its vertical component is Scosθ so that the total upward force due to it is 2πrScosθ . This balances the weight of a liquid cylinder of height h and weight πr2hρg , where ρ is the density of the liquid.
∴2πrScosθ=πr2hρg⇒h=rρg2Scosθ...........(1)
Diameter of the capillary tube = 0.4 mm
∴ Radius of the capillary tube, r=0.2 mm=0.2×10−3 m
(i) For water:
Surface tension of water, S=6.5×10−2 N/m
Contact angle, θ=0°
Density of water, ρ=1000 kg/m3
Substituting the values in Eq.(1),
h=0.2×10−3×1000×9.82×6.5×10−2×cos0° m⇒h=6.6×10−2 m⇒h=6.6 cm
(ii) For the liquid:
Surface tension, S=5.0×10−2N/m
Contact angle, θ=30°
Density of the liquid, ρ=800 kg/m3
∴h=0.2×10−3×800×9.82×5.0×10−2×cos30° m⇒h=5.5×10−2 m⇒h=5.5 cm
Answer: (i) Water rises to 6.6 cm in the capillary and (ii) the liquid rises to 5.5 cm
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